• Aucun résultat trouvé

The magnetosphere of the close accreting PMS binary V4046 Sgr AB

N/A
N/A
Protected

Academic year: 2021

Partager "The magnetosphere of the close accreting PMS binary V4046 Sgr AB"

Copied!
2
0
0

Texte intégral

(1)

Magnetic Fields throughout Stellar Evolution Proceedings IAU Symposium No. 302, 2013 P. Petit, M. Jardine & H. Spruit, eds.

c

 International Astronomical Union 2014 doi:10.1017/S1743921314001689

The magnetosphere of the close accreting

PMS binary V4046 Sgr AB

S. G. Gregory

1

, V. R. Holzwarth

2

, J.-F. Donati

3

, G. A. J. Hussain

4

,

T. Montmerle

5

, E. Alecian

6

, S. H. P. Alencar

7

, C. Argiroffi

8

,

M. Audard

9

, J. Bouvier

10

, F. Damiani

8

, M. G¨

udel

11

,

D. P. Huenemoerder

12

, J. H. Kastner

13

, A. Maggio

8

, G. G. Sacco

14

and G. A. Wade

15

1

School of Physics & Astronomy, University of St Andrews, St Andrews, KY16 9SS, U.K. email: sg64@st-andrews.ac.uk

2Freytagstr. 7, D-79114 Freiburg i.Br., Germany 3

Inst. de Recherche en Astrophysique et Plan´etologie UMR 5277, Toulouse, F31400 France

4

ESO, Karl-Schwarzschild-Str. 2, D-85748 Garching, Germany

5Institut d’Astrophysique de Paris, 98bis bd Arago, FR-75014 Paris, France 6

Obs. de Paris, LESIA, 5, place Jules Janssen, F-92195 Meudon Principal Cedex, France

7Dept. de F`ısica - UFMG, Av. Antˆonio Carlos, 6627, 30270-901 Belo Horizonte, MG, Brazil 8

INAF-Osservatorio Astronomico di Palermo, Piazza del Parlamento 1, I-90134 Palermo, Italy

9ISDC Data Center for Astrophysics, Univ. of Geneva, CH-1290 Versoix, Switzerland 1 0

UJF-Grenoble 1/CNRS-INSU, IPAG, UMR 5274, F-38041, Grenoble, France

1 1

Dept. of Astrophysics, University of Vienna, T¨urkenschanzstrasse 17, A-1180 Vienna, Austria

1 2MIT, Kavli Inst. for Astrophysics & Space Research, Cambridge, MA 02139, U.S.A. 1 3

CIS, Rochester Inst. of Technology, 54 Lomb Memorial Drive, Rochester, NY 14623, U.S.A.

1 4INAF-Arcetri Astrophysical Observatory, Largo Enrico Fermi 5, I - 50125 Florence, Italy 1 5

Dept. of Physics, Royal Military College of Canada, Kingston, K7K 7B4, Canada

Abstract. We present a preliminary 3D potential field extrapolation model of the joint

mag-netosphere of the close accreting PMS binary V4046 Sgr. The model is derived from magnetic maps obtained as part of a coordinated optical and X-ray observing program.

Keywords. stars: formation, stars: interiors, stars: magnetic field, stars: pre-main sequence

1. Introduction - large multi-wavelength observing campaign

V4046 Sgr is a close (separation∼ 9 R; Donati et al. 2011) circularised and synchro-nised PMS binary, accreting gas from a large circumbinary disk (Rosenfeld et al. 2012). It was observed as part of a coordinated X-ray and spectropolarimetric observing program with XMM-Newton and ESPaDOnS@CFHT during 2009. The observational highlights include: (i). the derivation of the first magnetic maps of a close accreting PMS binary system, see Fig. 1 (Donati et al. 2011). (ii). The detection of rotationally modulated soft X-ray emission associated with accretion shocks where accreting gas impacts the surface of the stars (Argiroffi et al. 2012). The modulation period is half of the binary orbital period. (iii). The realisation that V4046 Sgr may be a quadruple system, with GSC 07396-00759 a distant (projected separation∼12,350 au) companion to V4046 Sgr AB (Kastner

et al. 2011). The companion itself is likely a non-accreting PMS binary.

44

at https:/www.cambridge.org/core/terms. https://doi.org/10.1017/S1743921314001689

(2)

The magnetosphere of V4046 Sgr 45

Figure 1. Magnetic maps of the primary/secondary star of V4046 Sgr (left/middle respectively).

Blue/red is negative/postive field, with fluxes labelled in Gauss. Tick marks/numbers denote the phases of observation/rotation phase. The maps are shown in flattened polar projection with the bold circle/dashed lines the stellar equator/lines of constant latitude. Maps of the other field components & brightness/excess accretion-related emission maps can be found in Donati et al. (2011). The right panel shows a binary magnetic field extrapolation from the magnetic maps of V4046 Sgr. Only the large-scale field lines are shown. The magnetic fields are highly tilted with respect to the stellar rotation axes. Field lines connect through the interior of the binary from the nightside of one star to the dayside of the other.

2. The magnetic field of V4046 Sgr & field extrapolation

Magnetic maps of V4046 Sgr, derived from Zeeman-Doppler imaging, are shown in Fig. 1 (Donati et al. 2011). Only the radial field components are shown. Both stars are found to host complex large-scale magnetic fields with weak dipole components, consis-tent with their partially convective internal structure (Gregory et al. 2012).

A binary magnetic extrapolation is shown in Fig. 1. This has been constructed using a newly developed binary magnetic field extrapolation code that will be described in a forthcoming paper (Holzwarth in prep.). The code assumes that the large-scale field is potential and subject to three boundary conditions: the magnetic field is as measured from the maps at the surface of the each star, and a source surface boundary condition designed to mimic the pulling open of the large-scale magnetic loops by the stellar wind. The magnetic fields of both stars are linked, with loops connecting the dayside of one star to the nightside of the other. The field geometry, and the distribution of accretion columns and hot spots, will be detailed in a future paper (Gregory et al. in prep.).

Acknowledgements: SGG acknowledges support from the Science & Technology

Fa-cilities Council (STFC) via an Ernest Rutherford Fellowship [ST/J003255/1]. GAW is supported by a Discovery Grant from the Natural Science & Engineering Research Coun-cil of Canada (NSERC).

References

Argiroffi, C., Maggio, A., Montmerle, T., Huenemoerder, D. P., Alecian, E., Audard, M., Bouvier, J., Damiani, F., Donati, J.-F., Gregory, S. G., G¨udel, M., Hussain, G. A. J., Kastner, J. H., & Sacco, G. G. 2012, ApJ, 752, 100

Donati, J.-F., Gregory, S. G., Montmerle, T., Maggio, A., Argiroffi, C., Sacco, G., Hussain, G., Kastner, J., Alencar, S. H. P., Audard, M., Bouvier, J., Damiani, F., G¨udel, M., Huenemo-erder, D., & Wade, G. A. 2011, MNRAS, 417, 1747

Gregory, S. G., Donati, J.-F., Morin, J., Hussain, G. A. J., Mayne, N. J., Hillenbrand, L. A., & Jardine, M. 2012, ApJ, 755, 97

Kastner, J. H., Sacco, G. G., Montez, R., Huenemoerder, D. P., Shi, H., Alecian, E., Argiroffi, C., Audard, M., Bouvier, J., Damiani, F., Donati, J.-F., Gregory, S. G., G¨udel, M., Hussain, G. A. J., Maggio, A., & Montmerle, T. 2011, ApJL, 740, L17

Rosenfeld, K. A., Andrews, S. M., Wilner, D. J., & Stempels, H. C. 2012, ApJ 759, 119

at https:/www.cambridge.org/core/terms. https://doi.org/10.1017/S1743921314001689

Figure

Figure 1. Magnetic maps of the primary/secondary star of V4046 Sgr (left/middle respectively).

Références

Documents relatifs

While the Alliance has historically been engaged in the development of publications, videos and other materials that aim to demonstrate the worth of health policy and

That it holds for H 2 of the product of two smooth, projective varieties over an algebraically closed field, is a recent result of Skorobogatov and Zarhin, who used it in an

There is a motivation from logic : Were Z ⊂ Q diophantine, then Hilbert’s 10th problem over the rationals would have a negative answer (using Matijasevich’s theorem over Z).. Let

The Landau level ansatz, which is commonly accepted in non relativistic quantum mechanics as a good approximation for large magnetic fields, is a quite crude approximation for

Estimates in dimension d = 2 for constant magnetic fields Numerical results and the symmetry issue. 3 Magnetic rings: the one-dimensional periodic case Magnetic interpolation on

We observed from tongue contour tracings that the Mid Bunched configuration generally has a lower tongue tip than the Front Bunched one in speakers who present both bunched

Moreover we make a couple of small changes to their arguments at, we think, clarify the ideas involved (and even improve the bounds little).. If we partition the unit interval for

Homogeneous part: Weiss molecular field for magnetism Now, let’s consider N atoms: there are 2 N different configurations Hard to calculate Z and so the probability of a